Relation between H and B fields, and D and E fields

I am having some trouble understanding why the magnetic flux density B and the magnetic field strength H does not have the same units. I mean, as far as I understand, the H field is just the B field with the magnetic properties (magnetization) of the material taken into account? Isn't this correct? So why isn't the H field just the B field multiplied by some dimensionless scalar (or tensor)?

The same thing applies to the electric field E and the electric displacement D. If the D field is the electric field with the polarization taken into account, why do they not have the same units, and why is D not just E times some scalar value which depends on the polarizability of the material?

why is D not just E times some scalar value which depends on the polarizability of the material?

This is exactly how D is calculated! (although the polarisability is generally a matrix not a scalar).

The polarisability however has units, it is not a dimensionless quantity, so when we multiply some quantity by another, non-dimensionless (dimensioned?) quantity (i.e. multiplying E by polarisability), we must necessarily obtain a quantity that has different units.

So your question really boils down to "why does the polarisability have units?" In which case the answer should be fairly self-evident.

I am having some trouble understanding why the magnetic flux density B and the magnetic field strength H does not have the same units. I mean, as far as I understand, the H field is just the B field with the magnetic properties (magnetization) of the material taken into account? Isn't this correct? So why isn't the H field just the B field multiplied by some dimensionless scalar (or tensor)?

The same thing applies to the electric field E and the electric displacement D. If the D field is the electric field with the polarization taken into account, why do they not have the same units, and why is D not just E times some scalar value which depends on the polarizability of the material?

What you say is correct and is the basis for gaussian units. The use of SI units confuses the connection between the vectors E,D,B,H. SI was adopted about 50 years ago at an international congress, dominated (the hall was packed) by engineers who didn't understand the physics of electromagnetism.
Most elementary and intermediate texts use the confusing SI system, but working physicists more often use gaussian for their own calculations.
The 3rd ediltion of Jackson triles to go to SI, but even he as to use gaussian to complete the subject.

In gaussian units, charge and current are defined in absolute terms by the forces between two charges and between two wires.
Then there is no arbitrariness about their units.
1 stacoulomb=1 dyne-cm^2 from Coulomb's law.
1 statamp=1 sc/sec if the 1/c^2 is put into the force between two wires.
That connection (1/c^2) was measured by Weber and Kolrausch in 1856.
SI was developed 100 years ago because an engineer named Georgi thought that electric charge was a new unit, independent of force. Thus SI was originally called MKSA (A for ampere). Geogi did not know that there were other charges besides electric charge, and that after SR and QM physicists would realize that all charge (in terms of alpha) is dimensionless. Trying to give a dimension to an intrinsicly dimensionless quantity is why SI has a different unit for so many things (E,P,D,B,M,H) that should have the same unit. If SI can give units to empty space, then it would be equally sensible
(really nonesensical) to define the unit of charge as one newton if epsilonzero were given different arbitrary units than it has in SI.

Geogi did not know that there were other charges besides electric charge, and that after SR and QM physicists would realize that all charge (in terms of alpha) is dimensionless. Trying to give a dimension to an intrinsicly dimensionless quantity is why SI has a different unit for so many things (E,P,D,B,M,H) that should have the same unit. If SI can give units to empty space, then it would be equally sensible
(really nonesensical) to define the unit of charge as one newton if epsilonzero were given different arbitrary units than it has in SI.

Sorry don't fully follow here. I'm only used to the SI-system so this sounds interesting, can you please elaborate a little? Why is charge dimensionless for example?

Sorry don't fully follow here. I'm only used to the SI-system so this sounds interesting, can you please elaborate a little? Why is charge dimensionless for example?

In QED, the electron charge appears in the combination e^2/(hbar c).
(It would be divided by 4piepsilonzero in SI). Putting numbers in in ANY system gives the dimensionless number 1/137.036. This is called alpha and is the dimensionless charge value.

It seems strange however that E and D have different units in one system of units, and the same units in another one.

I mean, one could never define another system of units where a newton had the same units as coulomb, right?

you can define reality in terms of Planck Units and then every quantity measured really is unitless and dimensionless. (and the Gravitational constant, Speed of Light, and Planck's constant are all just the number 1, removing those scaling factors from the equations of physical law.)

from an SI point-of-view, D is measuring flux. think of this in terms of the natural meaning of an inverse-square action. we have a point charge Q "emmiting" a total quantity of flux that is the same as the amount of charge Q. these lines of flux are emmitted equally in all directions in 3 dimensional space.

the flux density is the density of these lines of flux per unit of area that is perpendicular to the lines of flux (perpendicular to the line connecting Q to that unit area). a sphere has a surface area of [itex] 4 \pi r^2 [/itex] so this total flux of Q is distributed equally among that entire surface area. that means that that the flux density, D, is the total flux, Q, divided by the total surface area [itex] 4 \pi r^2 [/itex] or

[tex] D = \frac{Q}{4 \pi r^2} [/tex]

or in vector form (assuming Q is at the origin)

[tex] \mathbf{D} = \frac{Q}{4 \pi | \mathbf{r} |^3} \mathbf{r} [/tex]

so flux density, D, is the physical quantity with dimension of charge per area or charge per square of length [Q][L]-2.

now the electrostatic field, E, is the physical quantity that represents how much force per unit charge that there is applied to a test charge, q, placed at position r from the main charge Q (which is at the origin). from the Coulomb Force equation we know that

In QED, the electron charge appears in the combination e^2/(hbar c).
(It would be divided by 4piepsilonzero in SI). Putting numbers in in ANY system gives the dimensionless number 1/137.036. This is called alpha and is the dimensionless charge value.

actually, Meir, we need to be clear about a couple of things. the most common name for this quantity is the Fine-structure constant and it is proportional to the square of the elementary charge, e. the other thing is that the expression

[tex] \alpha = \frac{e^2}{\hbar c} [/tex]

is only dimensionless (and currently believed to be 1/137.03599911) in unit systems that define the unit charge so that the Coulomb Force constant [itex] 1/(4 \pi \epsilon_0) [/itex] is 1 and disappears from the equations of physical law, namely the Coulomb force law (sorta like defining the unit force so that the constant C in [itex] F = C dp/dt [/itex] is 1 and goes away). this is an arbitrary human decision. in any system of units, the general expression for the Fine-structure constant is

[tex] \alpha = \frac{e^2}{\hbar c (4 \pi \epsilon_0)} [/tex] .

(i know you know this, Meir, but i think in introducing this to someone, one should not say simply "e^2/(hbar c)".)

one thing also to point out is that this Fine-structure constant really is the square of the elementary charge when measured in Planck units:

and can be thought of, in a world of natural units where all these scaling constants in the field equations go away, and given a constellation of charged bodies all with fixed numbers of protons and electrons in these charged bodies, that [itex] \alpha [/itex] represents the strength of the electromagnetic action.

BTW, Meir, i know that this is an old thread (and a different thread, but one of the issues are the same), i must say that i agree with you and marcusl fully about this. "H" should be called "flux" and "B" should be called "field".

You mean magnetic induction and field (flux is yet another quantity). Yes, many writers call B the magnetic field without explanation or comment. Mel Schwartz, in "Principles of Electrodynamics" (1972), is one of the few who are up front in addressing this:At this point we interject a small bit of philosophy. It is customary to call B the magnetic induction and H the magnetic field strength. We reject this custom inasmuch as B is the truly fundamental field and H is a subsidiary artifact. We shall call B the magnetic field and leave the reader to deal with H as he pleases.

actually, Meir, we need to be clear about a couple of things. the most common name for this quantity is the Fine-structure constant and it is proportional to the square of the elementary charge, e. the other thing is that the expression

[tex] \alpha = \frac{e^2}{\hbar c} [/tex]

is only dimensionless (and currently believed to be 1/137.03599911) in unit systems that define the unit charge so that the Coulomb Force constant [itex] 1/(4 \pi \epsilon_0) [/itex] is 1 and disappears from the equations of physical law, namely the Coulomb force law (sorta like defining the unit force so that the constant C in [itex] F = C dp/dt [/itex] is 1 and goes away). this is an arbitrary human decision. in any system of units, the general expression for the Fine-structure constant is

[tex] \alpha = \frac{e^2}{\hbar c (4 \pi \epsilon_0)} [/tex] .

(i know you know this, Meir, but i think in introducing this to someone, one should not say simply "e^2/(hbar c)".)

one thing also to point out is that this Fine-structure constant really is the square of the elementary charge when measured in Planck units:

and can be thought of, in a world of natural units where all these scaling constants in the field equations go away, and given a constellation of charged bodies all with fixed numbers of protons and electrons in these charged bodies, that [itex] \alpha [/itex] represents the strength of the electromagnetic action.

I am puzzled by your post, since I assume you read mine that you quote, and I think we are in almost complete agreement.
1. The term "fine structure constant" is the historical designation because it was first noted in atomic spectrocopy 100 years ago. Now that we know that alpha is a standard ratio between many numbers in physics, it is probably time to not limit it to fine structure, and just call it alpha, but that is not an important point.
2. I did mean to imply that alpha had somewhat different algebraic forms
in different systems of units. That is why I explicity mentioned the division by
fourpiepsilonzero in SI. I did not mention, but should have that it is simplest in the form of natural units used today by most HE theorists, where
alpha=e^2. Fortunately, I know of no one (you and I included) who redefines alpha to be anything other than 1/137. e^2, on the other hand, has many different values in different unit systems.
3. I am glad we both agree that "[itex] \alpha [/itex] represents the strength of the electromagnetic action". I would only add: whatever system of units is used.
Thank you for your interest.

you can define reality in terms of Planck Units and then every quantity measured really is unitless and dimensionless. (and the Gravitational constant, Speed of Light, and Planck's constant are all just the number 1, removing those scaling factors from the equations of physical law.)

from an SI point-of-view, D is measuring flux. think of this in terms of the natural meaning of an inverse-square action. we have a point charge Q "emmiting" a total quantity of flux that is the same as the amount of charge Q. these lines of flux are emmitted equally in all directions in 3 dimensional space.

the flux density is the density of these lines of flux per unit of area that is perpendicular to the lines of flux (perpendicular to the line connecting Q to that unit area). a sphere has a surface area of [itex] 4 \pi r^2 [/itex] so this total flux of Q is distributed equally among that entire surface area. that means that that the flux density, D, is the total flux, Q, divided by the total surface area [itex] 4 \pi r^2 [/itex] or

[tex] D = \frac{Q}{4 \pi r^2} [/tex]

or in vector form (assuming Q is at the origin)

[tex] \mathbf{D} = \frac{Q}{4 \pi | \mathbf{r} |^3} \mathbf{r} [/tex]

so flux density, D, is the physical quantity with dimension of charge per area or charge per square of length [Q][L]-2.

now the electrostatic field, E, is the physical quantity that represents how much force per unit charge that there is applied to a test charge, q, placed at position r from the main charge Q (which is at the origin). from the Coulomb Force equation we know that

1. The term "fine structure constant" is the historical designation because it was first noted in atomic spectrocopy 100 years ago. Now that we know that alpha is a standard ratio between many numbers in physics, it is probably time to not limit it to fine structure, and just call it alpha, but that is not an important point.

but the name is there. it's what you use to look up the concept, even if it is now known that this concept sorta trancends the fine-structure splitting.

2. I did mean to imply that alpha had somewhat different algebraic forms in different systems of units. That is why I explicity mentioned the division by fourpiepsilonzero in SI.

i know i'm swimming against the trend, but i still think that the general expression (not just for SI) should be

[tex] \alpha = \frac{e^2}{\hbar c (4 \pi \epsilon_0)} [/tex]

and then just note that [itex] 4 \pi \epsilon_0 [/itex] gets set to 1 in some systems of units because of the manner that the unit charge is defined in those systems of units. personally, i think it's much more natural to define charge so that [itex] \epsilon_0 = 1 [/itex] (and, for gravitation set [itex] 4 \pi G = 1 [/itex]) and then (with [itex] c = \hbar = 1 [/itex]) you get [itex] \sqrt{4 \pi \alpha} = e [/itex] which i think is the more natural and salient dimensionless number for which \alpha is derived.

3. I am glad we both agree that "[itex] \alpha [/itex] represents the strength of the electromagnetic action". I would only add: whatever system of units is used.

that's true, but hard to conceptualize without thinking in terms of natural units. the gravitational attraction between two planets exceeds the electrostatic repulsion if they happened to be equally charged by a few elementary charges. without going to natural units, comparing the magnitude of actions from different fundamental forces is like comparing apples to oranges. electromagnetics operates on charge and gravitation (in the Newtonian sense) operates on mass. when you compare the two actions, how much charge do you use in comparison to how much mass?

From a more abstract viewpoint, H and B aren't even the same type of geometrical object. H is a [twisted-]1-form in space, which is associated with a line-integral, and B is a 2-form in space, which is associated with a surface-integral. Similarly, E is a 1-form and D is a [twisted-]2-form.

I think this post, compared my sentence "What you say is correct and is the basis for gaussian units." presents the case for using gaussian rather than SI units.

fine. but why stop there? continuing the "let's get rid of scaling constants" impetus, why not go all the way to Planck Units? personally, i think the [itex] 4 \pi [/itex] constants should also be lost, also, when using Gauss's law for either electrostatics or for gravitation and then you get field equations with no scaling constants except for an occasional "2".

BTW, Meir, i know that this is an old thread (and a different thread, but one of the issues are the same), i must say that i agree with you and marcusl fully about this. "H" should be called "flux" and "B" should be called "field".

rbj, there's reason to call B "field," but please don't call H "flux" because this is a different quantity as I had noted earlier in the thread you quoted. Magnetic flux is defined by
[tex]\Phi = \int \vec{B} \cdot d\vec{A}[/tex]
and has units of Webers (SI) or Maxwells (Gaussian/cgs).

It might be better to join authors such as E. Weber and Julius Stratton who call H "magnetic intensity."

rbj, there's reason to call B "field," but please don't call H "flux" because this is a different quantity as I had noted earlier in the thread you quoted. Magnetic flux is defined by
[tex]\Phi = \int \vec{B} \cdot d\vec{A}[/tex]
and has units of Webers (SI) or Maxwells (Gaussian/cgs).

It might be better to join authors such as E. Weber and Julius Stratton who call H "magnetic intensity."

okay, i meant to call H "flux density" like we call D. i know we call B "flux density" because

[tex]\Phi = \int \vec{B} \cdot d\vec{A}[/tex]

but, if E is "field" (because it is related to intensity of effect) and D is "flux density" (because it is related to the density of how much of the source of the effect is present at some point), to be consistent, shouldn't they have named "H" as "magnetic flux density" and "B" as "magnetic field"? isn't calling "B" a flux density an historical accident?

okay, i meant to call H "flux density" like we call D. i know we call B "flux density" because

[tex]\Phi = \int \vec{B} \cdot d\vec{A}[/tex]

but, if E is "field" (because it is related to intensity of effect) and D is "flux density" (because it is related to the density of how much of the source of the effect is present at some point), to be consistent, shouldn't they have named "H" as "magnetic flux density" and "B" as "magnetic field"? isn't calling "B" a flux density an historical accident?

No, because E and B are the fundamental field quantities, while D and H are derived [Jackson] "as a matter of convenience to take into account in an average way the contributions ... of atomic charges and currents." That is why E and B should be called fields, and why Mel Schwartz doesn't bother to even name H in his book. Furthermore, D is almost universally called Electric Displacement, and only rarely "dielectric flux density."

From a more abstract viewpoint, H and B aren't even the same type of geometrical object. H is a [twisted-]1-form in space, which is associated with a line-integral, and B is a 2-form in space, which is associated with a surface-integral. Similarly, E is a 1-form and D is a [twisted-]2-form.

Can you elaborate on this for those of us who are differential-geometrically-challenged? I am lost by even the introduction (for instance the authors state that E&M is independent of gravitation, yet the field tensor F in eqs. (2)-(3) would seem to depend explicitly on g).

From a more abstract viewpoint, H and B aren't even the same type of geometrical object. H is a [twisted-]1-form in space, which is associated with a line-integral, and B is a 2-form in space, which is associated with a surface-integral. Similarly, E is a 1-form and D is a [twisted-]2-form.

Can you elaborate on this for those of us who are differential-geometrically-challenged? I am lost by even the introduction (for instance the authors state that E&M is independent of gravitation, yet the field tensor F in eqs. (2)-(3) would seem to depend explicitly on g).

In that paper, eqs (2) and (3) are a set of metric-dependent equations that appear in the Einstein paper referenced there. Actually in each set, the metric appears explicitly only in the "constitutive" equation relating the [tex]\cal F[/tex] tensor and the tensors [tex]F[/tex] (in 2) and [tex]\phi[/tex] (in 3). The story of formulating electromagnetism without a metric starts in part IV. A key idea is that there are two independent field tensors that capture most of electromagnetism. In the presence of a metric or other structure, the two tensors are related... possibly to the point where they are not easily distinguishable.